Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 CHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 The DØ Detector for Run II Levan Babukhadia SUNY at Stony Brook for the DØ Collaboration SUNY at Stony Brook for the DØ Collaboration

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Physics Challenges  The Upgraded Tevatron Interactions / xing Bunch xing (ns)  Ldt (pb -1 /week) 5.2    Typical L (cm -2 s -1 )  s (TeV) 140   366  6 Bunches in Turn Run 2bRun 2aRun 1b Run 1  Run 2a  Run 2b 0.1 fb -1  2  4 fb -1  15 fb -1 Peak Lum. achieved over 2  cm  2 s  1 Planned to reach Run 2a design by Spring 2003 Physics goals for Run 2  precision studies of weak bosons, top, QCD, B-physics  searches for Higgs, supersymmetry, extra dimensions, other new phenomena require  electron, muon, and tau identification  jets and missing transverse energy  flavor tagging through displaced vertices and leptons  luminosity, luminosity, luminosity…

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 New tracking devices, Silicon (SMT) and Fiber Tracker (CFT), placed in 2 T magnetic field (see also George Ginther’s talk in this session) Upgraded Calorimeter electronics readout and trigger SMT Added PreShower detectors, Central (CPS) and Forward (FPS) Significantly improved Muon System New forward proton spectrometer (FPD) Entirely new Trigger System and DAQ to handle higher event rate Physics Challenges  The Upgraded Detector

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 LAr in gap 2.3 mm Ur absorber Readout Cell Cu pad readout on 0.5 mm G10 with resistive coat epoxy Drift time ~430 ns North End Cap South End Cap Central Cal. ICD EM FH CH OH MH IHEM MG FPS Calorimeters Liquid Argon sampling uniform response, rad. hard, fine spatial segmentation LAr purity important Uranium absorber (Cu/Steel CC/EC for coarse hadronic) nearly compensating, dense  compact Uniform, hermetic with full coverage |  | < 4.2 (   2 o ), int ~ 7.2 (total) Single particle energy resolution e:  /E = 15% /  E  0.3%  :  /E = 45% /  E  4%  50k readout cells (< 0.1% bad)  Fine segmentation  5000 pseudoprojective towers ( 0.1  0.1 )  4 EM layers, shower-max (EM3): 0.05  0.05  4/5 Hadronic ( FH + CH )  L1/L2 fast Trigger readout 0.2  0.2 towers  Fully commissioned

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 DØ Run 2 Preliminary J/   ee M = 2.98 GeV  = 166 MeV   Three-jet event E T jet1 ~ 310GeV, E T jet2 ~ 240GeV E T jet3 ~ 110GeV, E T ~ 8GeV Z  ee employed for EM calibration E T from multijet data DØ Run 2 Preliminary  (E T )~7GeV Present performance of  (E T ) from incl. di-electrons with at least one track match (mainly Z, Drell-Yan) Calorimeter Performance

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Muon System Fully commissioned Bottom B/C Scintillators A-  Scint PDTs Forward Tracker (MDTs) Shielding Forward Trigger Scintillators Central and Forward regions, coverage up to  = ± 2 Three layers: one inside (A), two outside (B, C) the toroid magnets Consists of scintillators and drift tubes Central Proportional Drift Tubes (PDT’s) 6624 drift cells (10.1  5.5 cm) in 94 three- and four-deck chambers Central Scintillation Counters 360 “cosmic ray” counters outside the toroid (  = 22.5  ) 630 “A  ” counters inside (  = 4.5  ),  = 0.1 Forward Mini Drift Tubes (MDT’s) cell tubes in 8 octants per layer on North and South side, cell cross-section 9.4  9.4 mm Forward Scintillation Counters (Pixels) 4214 counters on the North and South side  = 4.5  matches the MDT sector size

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Muon System Performance Muon Timing Cosmic rays  ’s from Collisions Timing cuts reduce cosmic bckg., could aid in detection of slow moving particles Z   +   candidate M = 3.08  0.04 GeV  = 0.78  0.08 GeV Muon stand alone systemMuon plus central tracking J/  invariant mass Matching of central tracks to  ’s improves momentum resolution CHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 D S Q 4 Q 3 Q 2 S A1A1 A2A2 P1P1 P2P2 p p z (m) D 2 D 1 A2A2 Q 2 Q 3 Q  Routinely insert pots during collisions  Recorded > 2 M elastic events with stand-alone DAQ  Working on integration of FPD with the rest of DØ  First diffractive+jet data by December DØ Forward Proton Detector  Diffractive and elastic physics program  need special detectors at very small angles: FPD  FPD consists of 2 arms (outgoing proton and anti-proton)  18 Roman pots in 4 quadrupole and 2 dipole “castles”  From hits in scintillating fiber detectors installed in Roman pots  fractional energy lost by the proton and scattering angle  trigger on elastic, diffractive, double pomeron events Dipole Castle

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 DØ Trigger System L3/DAQ Tape 2.3 (7.5) MHz 5 kHz 1 kHz L3 Trigger 50 Hz Decision times: ~4.2  s ~100  s ~50 ms Level 1 Subdetectors Towers, tracks, clusters, E T Some correlations Pipelined Level 2 Correlations Calibrated Data Separated vertex Physics Objects e, , j, , E T Level 3 Simple Reconstruction Physics Algorithms Entire Trigger Menu configurable and downloadable at Run start Trigger Meisters provide trigger lists for the experiment by collecting trigger requests from all physics groups in the Trigger Board All past and present trigger lists are stored and maintained in the dedicated trigger database

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Implemented in ~100 digital boards with same motherboard and different flavors of daughter- cards with over 500 Xilinx Virtex FPGAs Provides charged lepton id in Level 1 by finding tracks in 4.5  azimuthal trigger sectors of CFT Helps with EM-id in Level 1 by reconstructing clusters of energy in CPS scintillator strips Helps with Muon-id in Level 1 by sending 6 highest p T tracks to L1Muon in about 900ns Helps with EM-id in forward regions |  | < 2.6 by reconstructing clusters of energy in FPS strips Helps with charged lepton id in forward regions by confirmation in pre-radiator layers of FPS Facilitates matching of preshower and calori- meter objects at quadrant level Helps with displaced vertex id in Level 2 Silicon Track Trigger by providing the Level 1 CFT tracks for global SMT+CFT track fitting Currently being commissioned DØ Track and Preshower Digital Trigger

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Data Acquisition System DØ Detector 1 kHz Tape ~250 kB/event Gathers raw data from the front-end crates following each Level 2 Accept Based on “off the shelf” components Single Board Computers (SBCs) read out Level 3 buffers: Intel 1GHz, VME based, dual 100Mb Ethernet, Linux OS SBCs send data to a Level 3 node over fast Ethernet switches according to instructions received from the Routing Master The routing Master program runs on an SBC in a special crate receiving data from the Trigger Framework Cisco Switch sends data to Linux Level 3 Farm nodes Event building and Level 3 trigger selections performed by 48-node Linux farm

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Level 1 and Level 2 Trigger Performance Rate (Hz) Luminosity (10 30 cm -2 s -1 ) central forward Level 1 Calorimeter Jet and EM trigger “turn-on”s Level 1 Muon trigger rate dependence on Luminosity Level 2 Calorimeter Jet and EM trigger efficiencies Level 2 Muon trigger efficiency and rejection L2EM(1,10 GeV; EMF > 0.85) L2JET(1,10 GeV) Jet EM

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Level 3 Trigger Performance Level 3 Jet Tool “turn-on” Considered Passed Offline EM E T (GeV) 15 GeV L3 EM Trigger Rej.~10 w.r.t. to L1 (10 GeV at L1) 12 GeV + shower shape cuts.OR. the above The 48-node Linux Level 3 farm working and selecting events, by triggering on Jets, EM objects, Muons, Taus

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 DØ Detector Run 2b Upgrade Trigger Upgrade Upgrade L1 Track Trigger to narrow roads, improve Track-Cal. matching Upgrade L1/2 Cal. Trigger to use digital filter, isolation, shape cuts Incremental upgrades to Level 2, Level 3 Triggers and online system Present detector was designed for ~2  4fb  1 integrated and ~2  cm  2 s  1 instantaneous Luminosity Run 2b goal ~15fb  1 before LHC Physics  Physics motivations: Higgs and Supersymmetry  Exceeds radiation tolerance of existing Silicon detector  Requires higher instantaneous luminosities, ~5  cm  2 s  1, trigger upgrades Silicon Upgrade Replace Silicon Detector with a more radiation-hard version New Silicon tracker with innermost layer at 1.78 cm (c.f in Run 2a) Maintain good pattern recognition coverage |  | < 2

Levan BabukhadiaICHEP02 – 31 st International Conference on High Energy Physics, Amsterdam, 24 – 31 July, 2002 Summary and Outlook The DØ Detector for Run 2 is operating and collecting physics data Enormous progress over the past year in installation, integration, commissioning of the detector and understanding the data Performance of the Run 2 DØ detector is very encouraging all subdetectors are operating well software and computing systems are working well we are reconstructing electrons, muons, jets, missing E T, J/ , W’s and Z’s and first results already presented at winter/spring and now at summer conferences We are working hard on what still needs to be done complete commissioning of Level 1 Track Trigger improve calibration and alignment integrate Level 2 Silicon Track Trigger later this year optimize detector, trigger, and DAQ performance continue working on Run 2b Upgrade Project We are on the way to exciting physics, first physics results coming soon, exciting years are ahead!